Resumen de: CN122696179A
一种基于波函数文件的分子描述符自动提取解析与机器学习数据集构建方法,涉及计算化学数据处理与材料信息技术领域。包括:1)递归扫描分子文件夹,识别量子化学计算文件,建立分子数据对象;2)根据文件格式特征自动识别量化计算程序类型,并提取计算参数与结果等信息;3)按照预设优先级自动选择不同波函数文件,并调用Multiwfn进行静默批处理;4)自动提取30余种电子结构描述符,并与分子基础信息、目标标签和文件来源进行统一存储、匹配、合并和格式规整,输出可直接用于机器学习的标准化数据集。本发明能够实现不同来源量子化学计算结果的自动识别、解析以及机器学习数据集自动构建,提高大规模分子电子结构数据处理效率,降低人工整理误差。
Resumen de: CN122693873A
本发明涉及一种相干伊辛机的泵浦时序控制方法及相关设备。方法包括:获取待求解问题的耦合矩阵,以提取问题特征向量;在相干伊辛机运行过程中,实时采集当前演化状态;将问题特征向量与当前演化状态融合为当前状态向量,并输入至目标强化学习策略网络;目标强化学习策略网络采用仿真预训练与硬件迁移学习相结合的方式离线训练得到,输入层维度与当前状态向量的维度匹配,输出层维度与泵浦控制参数的维度匹配;利用目标强化学习策略网络根据当前状态向量,输出用于调节相干伊辛机的泵浦控制参数对应的数值,以生成适配于待求解问题的非单调泵浦时序。该方法达到了提升泵浦时序控制的灵活性和适应性,提升求解质量、提高求解效率的技术效果。
Resumen de: CN122693875A
本发明提供了一种超导量子比特的多路复用控制系统,属于量子领域,该多路复用控制系统包括:第一微波源,用于输出控制信号;第二微波源,用于输出偏置信号;寻址选择机构;M个可调超导滤波器与寻址选择机构的M个输出部以及M个超导量子比特一一对应的连接;传输机构与M个可调超导滤波器连接;寻址选择机构适用于将控制信号路由至与任一超导量子比特连接的可调超导滤波器,传输机构将偏置信号路由至可调超导滤波器,偏置信号用于将可调超导滤波器的滤波频率配置为与超导量子比特的工作频率相匹配,以对控制信号滤波,滤波后的控制信号用以操控超导量子比特,本发明的多路复用控制系统使超导量子处理器的具有可扩展性。
Resumen de: CN122693881A
本发明涉及一种本发明公开了一种光量子芯片的校准方法、装置、系统及介质,该方法包括:针对当前规模的热串扰矩阵,计算各热光调控单元的驱动补偿值;在施加补偿值的条件下运行芯片,并监测表征相位漂移的状态量;当状态量超出预设阈值时,对该热串扰矩阵进行降维处理,获得规模更小的热串扰矩阵;将降维后的矩阵更新为当前矩阵,并递归执行上述步骤。本发明通过递归降维,将高维校准问题分解为低维子问题,显著降低了计算复杂度,缩短了校准时间。
Resumen de: CN122698015A
本申请公开了一种高饱和功率的约瑟夫森参量放大器及其封装结构,涉及量子计算技术领域。本发明具体包括:阻抗匹配单元、非线性谐振单元和磁通调节单元;非线性谐振单元与阻抗匹配单元连接,其包括并联的电容部件和直流超导量子干涉器件;直流超导量子干涉器件包括两条并联连接的串联结支路,每个串联结支路包含多个相互串联的约瑟夫森结;磁通调节单元与直流超导量子干涉器件耦合,提供磁通偏置信号和磁通泵浦信号。本发明通过在直流超导量子干涉器件中引入级联的约瑟夫森结,解决了传统放大器在多比特读取时单个约瑟夫森结非线性过载及增益压缩的问题。
Resumen de: CN122693879A
本公开涉及计算机技术领域,特别涉及一种测量方法、装置及设备,存储介质,程序产品,包括:对二维纳米结构的第一类边界施加磁场,其中,所述二维纳米结构包括所述第一类边界和第二类边界,所述二维纳米结构与超导体近邻耦合;分别在不同磁场强度下,测量所述二维纳米结构的多个角点中每个角点处的局域电导和所述多个角点中不同角点之间的非局域电导,其中,所述多个角点包括所述第一类边界和所述第二类边界之间的交点;根据所述局域电导、所述非局域电导在不同磁场强度下的测量结果,确定所述多个角点处的能态,所述测量结果包括所述非局域电导随磁场强度的变化趋势。
Resumen de: CN122691427A
本申请实施例提供了一种电压校准参数确定方法、前端服务单元、测控系统和介质。方案如下:获取AWG板卡对应所有通道的第一通道信息,并在前端服务页面显示第一通道信息;基于用户在前端服务页面针对目标通道和第一整数触发的第一初始化操作,获取第一电压;基于用户在前端服务页面针对目标通道和第二整数触发的第二初始化操作,获取第二电压;基于第一电压、第二电压和预设电压阈值,计算目标通道的第二校准参数,并将前端服务页面中目标通道对应第二通道信息中的第一校准参数更新为第二校准参数。通过本申请实施例提供的技术方案,实现AWG板卡电压校准过程校准参数的确定,为AWG板卡关闭重启时的电压校准过程提供保障。
Resumen de: CN122693728A
本发明公开了基于量子主方程的扩散模型概率流演化方法、系统及介质,涉及量子技术领域,包括:将扩散过程中当前时间步的中间概率分布编码为量子态,并在量子处理单元上制备所述量子态;根据扩散模型的Fokker‑Planck方程构造对应的量子主方程,在量子处理单元上利用量子主方程对所述量子态进行演化,得到演化后的量子态;对所述演化后的量子态进行量子测量,获得测量结果;根据所述测量结果计算分布损失,并利用所述分布损失更新经典去噪网络的参数;该方法提升了高维概率分布演化的精度,减少了采样步数,提高了推理效率。
Resumen de: CN122691657A
本申请实施例提供了一种参数配置方法及前端服务设备。方案如下:根据用户在前端服务页面针对任务处理设备触发的参数配置操作,获取任务处理设备的参数配置文件,参数配置文件中包括量子计算测控系统对应的类型、机箱信息、通道信息、地址信息和电压校准数据,以及任务处理设备的编译解析信息;将参数配置文件存储至预设缓存器,以使任务处理设备从预设缓存器中获取参数配置文件进行参数配置。通过本申请实施例提供的技术方案,实现了任务处理设备的参数配置。
Resumen de: CN122698226A
本发明涉及深度学习,具体涉及一种基于量子光学的安全多方深度学习系统及方法,服务器,将待保护的神经网络权重编码为相干光态发送至客户端,并通过分析客户端返回的验证态的噪声特征计算权重信息的泄露上界;客户端,接收服务器发送的相干光态,通过依次执行第一幺正变换、基于可调增益的放大与分束、第二幺正变换来计算内积,该内积用于激活本地神经网络,同时将计算内积时引入的额外量子噪声通过第二幺正变换弥散至所有模式后,生成并返回一个验证态至服务器,客户端根据可调增益计算数据信息的泄露上界;本发明提供的技术方案能够有效克服现有技术所存在的深度学习推理过程中难以兼顾模型权重与用户数据双向隐私保护的缺陷。
Resumen de: JP2026141692A
0001 【課題】誤り耐性のある量子計算を効率的に行うこと。 【解決手段】本開示の一態様による量子計算装置は、表面符号とHGP符号とを組み合わせて誤り耐性のある量子計算を実現する量子計算装置であって、所定の形式で表現された第1の量子プログラムをπ/8回転形式で表現した第2の量子プログラムに変換する変換部と、前記第2の量子プログラムに含まれる第1の命令と、前記表面符号により符号化されている論理量子ビットと、前記HGP符号により符号化されている論理量子ビットとに基づいて、前記HGP符号の論理量子ビットで実行可能な第2の命令に前記第1の命令を変換する変換部と、シャトリングを利用して前記第2の命令が表す前記量子計算を実現する量子計算部と、を有する。 【選択図】図3
Resumen de: WO2025162852A1
Disclosed is a Josephson junction traveling-wave parametric circuit (100) comprising unit cells (1101) which are coupled in series to form a transmission line between an input port (PIN) and an output port (POUT)- Each unit cell comprises a series Josephson junction (Ji) and a dispersive ground-shunt admittance (112i), particularly comprising a capacitive element (Ci) and an inductive element (Li) adding dispersion, configured to cause suppression of one or more sideband frequency components. The circuit may be a Josephson traveling- wave parametric amplifier (JTWPA), particularly for amplifying a readout signal of a quantum bit.
Resumen de: US2022014277A1
0001 A photon source module includes a plurality of photon sources, wherein each photon source is configured to non-deterministically generate one or more non-entangled or entangled photons in response to receiving a trigger signal. When two or more photon sources simultaneously generate photons in response to a trigger signal, one photon of a first photon pair is directed to a photon processing system and one photon of a second photon pair is directed to a photon analyzer. During repetitive operation, the photon analyzer analyzes photons from each of the plurality of photon sources to determine characteristics of each photon source and can use that information to direct the highest quality photons to the photon processing system.
Resumen de: US20250079034A1
Example embodiments provide quantum computers, laser light delivery systems for quantum computers, and methods for delivering laser light from lasers of quantum computers to atomic object confinement apparatuses of quantum computers. In an example embodiment, a quantum computer comprises an atomic object confinement apparatus, a laser, a cylindrical guide positioned such that a first end of the cylindrical guide is adjacent the laser and a second end of the cylindrical guide is adjacent the atomic object confinement apparatus, and an optical fiber cable helically wrapped around the cylindrical guide and spanning from the first end to the second end. The optical fiber cable is configured to deliver laser light generated by the laser to the atomic object confinement apparatus. A pitch of the helically wrapped optical fiber cable is selected to provide a desired effective bend radius of the optical fiber cable to strip higher-order modes of the laser light.
Resumen de: US20260260153A1
One or more properties of a quantum error correction protocol are specified in a formal language using a theorem prover. A quantum error correction protocol and a formal proof certificate are synthesized, the formal proof certificate being a machine-checkable proof that the quantum error correction protocol satisfies the one or more properties. The quantum error correction protocol is compiled into a quantum circuit with the formal proof certificate embedded in the quantum circuit. The quantum circuit is deployed onto quantum computing hardware.
Resumen de: US20260259854A1
Disclosed in the present disclosure are a quantum operation processing method, apparatus, and system. The above solution relates to the quantum technical field. The method includes: receiving a control instruction from a processor, where the control instruction is configured to indicate to perform a quantum operation on a plurality of quantum devices; based on the control instruction, acquiring a quantum operation instruction from a storage device externally mounted on the processor; and determining a plurality of target electronic devices corresponding to the quantum operation instruction, where the plurality of target electronic devices are respectively configured to generate, based on the quantum operation instruction, a waveform signal for performing the quantum operation on the corresponding quantum devices.
Resumen de: US20260260152A1
A computer-readable recording medium stores therein a program for causing a computer to execute a process, the process including: calculating energy of a molecule based on energy of each of multiple fragments obtained by dividing a structure of the molecule by a molecule dividing method, the calculating including: estimating, for each of the multiple fragments, a candidate value from which noise has been removed, based on multiple candidate values that are calculated by a variational quantum eigenvalue solver, each of the multiple candidate values being calculated for each of a multiple parameters of a first variational quantum circuit representing a Hamiltonian of the each of the multiple fragments, the each of the multiple candidate values being a potential solution of the parameter; and calculating, for each of the multiple fragments, an energy thereof based on the candidate value from which noise has been removed and estimated for each of the multiple parameters.
Resumen de: US20260260142A1
A method may include generating directed graphs, each of the directed graphs representing a quantum circuit. The method may also include evaluating each of the directed graphs according to operation of the quantum circuit represented by each of the directed graphs. The method may include selecting one of the directed graphs based on the evaluations. The method may further include transforming the selected directed graph to generate a second directed graph.
Resumen de: US20260260776A1
0000 The invention relates to neutral atom quantum computers having a zoned architecture that includes a storage zone and an interaction zone as part of an array of atoms that form the quantum register in an optical lattice. A schedule optimizer determines an optimized atom schedule for moving atoms between the storage zone and the interaction zone using optical tweezers generated by an optical trap generator responsive to the optimized atom schedule. The schedule optimizer may be implemented according to several variations of algorithms that include an annealing solver and a mathematical optimization engine. The schedule optimizer receives an objective function that includes selectable factors that correlate to minimizing the logical error rate for a set of operational tasks, various hardware constraints such as zone geometries and circuit schedules.
Resumen de: US20260260144A1
Examples of the present disclosure are directed to a method for operating a quantum computing system (QCS) to load classical data. The method includes configuring a quantum circuit to implement a target classical function that is defined over a string of input bits. The target classical function is decomposed into a set of parity sub-functions. A set of quantum registers of the QCS is initialized with a superposition of input states corresponding to the string of input bits. A sequence of Quantum Read-Only Memory (QROM) operations is executed on the set of quantum registers to generate a set of outputs. Each QROM operation of the sequence of QROM operations encodes a separate parity sub-function of the set of parity sub-functions. Each output of the set of outputs is routed to a separate output register of a set of output registers of the QCS.
Resumen de: WO2026180934A1
In a method for implementing a Clifford gate on a quantum hardware system, a symplectic matrix representation of the Clifford gate is determined that factorizes as a product comprising at least five matrices alternating between matrices corresponding to X-diagonal Clifford operators and matrices corresponding to Z-diagonal Clifford operators. The Clifford gate is synthesized into a sequence of quantum gates, based on the symplectic matrix representation of the Clifford gate. The method comprises causing the quantum hardware system to implement the sequence of quantum gates.
Resumen de: US20260260711A1
0000 A non-transitory computer-readable recording medium stores therein a program that causes a computer to execute a process including dividing a molecule into a plurality of fragments, calculating, for each of the fragments, a first eigenvalue for each of bath orbitals included in the fragments, calculating a second value for each of the bath orbitals based on the first eigenvalue, sorting the second values in a descending order and deriving a cumulative distribution function of the second values, determining the number of the bath orbitals for which a cumulative probability of the cumulative distribution function is greater than a predetermined threshold value, selecting the bath orbitals corresponding to the second values from a largest one among the second values sorted in the descending order, in the number equal to the determined number of the bath orbitals, and calculating an energy of the molecule using the selected bath orbitals.
Resumen de: US20260260199A1
0000 The present disclosure provides a method of facilitating automated regulatory compliance determination. Further, the method may include receiving, using a communication device, a compliance input data from a regulatory data source. Further, the method may include receiving, using the communication device, an operational input data from an enterprise system. Further, the method may include determining, using a processing device, a compliance status data by processing the compliance input data and the operational input data using a quantum-inspired neural network. Further, the method may include generating, using the processing device, a compliance output data based on the compliance status data. Further, the method may include storing, using a storage device, the compliance output data. Further, the method may include transmitting, using the communication device, the compliance output data to a client system.
Resumen de: WO2026180792A1
A quantum error correction method and quantum computing system are disclosed. The quantum computing system receives syndrome data and sets defect states of nodes in a decoding hypergraph according to defects identified in the syndrome data. The quantum computing system determines a plurality of decoding windows associated with logical observable subsets of a logical observable and independently decodes the decoding windows to determine partial corrections. The partial corrections are then combined by the quantum computing system to determine an aggregate correction for an error state of quantum devices in the quantum computing system.
Nº publicación: US20260260145A1 03/09/2026
Solicitante:
ATLANTIC QUANTUM CORP [US]
Atlantic Quantum Corp.
Resumen de: US20260260145A1
0000 Techniques are described for controlling qubits using baseband pulse sequences. Many, or even all, qubits in a system can be controlled by baseband pulse sequences that are synchronized to a clock signal shared by the qubits. The baseband pulse control techniques allow many qubits to be driven with the same parameterized baseband pulse sequence applied based on a common clock signal, with parameters of the baseband pulse sequence selected based on the desired operation. This approach greatly simplifies the electronics needed to drive a collection of qubits, as there is no need for picosecond timing, nor the complexities that arise from varied gate durations.